Unit 7, lesson 91

Polar Graphs of Roses and Lemniscates

How the petal count of a rose depends on whether its angular frequency is odd or even, how negative radii draw petals on the far side, and which angles give real points on a lemniscate.

  • Theory part 181
  • Practice part 182
  • Polar Graphs

Wrap the graph of r=cos⁡2θr = \cos 2\theta around the pole and it opens into four petals. Change the 22 to a 33 and you get three petals, not six. The difference comes from negative radii, which sometimes draw new petals and sometimes land exactly on old ones. A close relative, the lemniscate, has a squared radius, and there the first question is which angles give any real points at all.

Key terms

Rose curves

Definition Let a≠0a \ne 0 and let n≥2n \ge 2 be an integer. The graphs of

r=acos⁡(nθ)andr=asin⁡(nθ)r = a\cos(n\theta) \quad \text{and} \quad r = a\sin(n\theta)

are rose curves. The curve consists of petals. Each petal starts and ends at the pole, is drawn by the angles between two consecutive zeros of the radius, which are πn\frac{\pi}{n} apart, and reaches out to distance ∣a∣\lvert a \rvert at its tip. For n=1n = 1 the same equations give circles through the pole, not roses.

In plain words As θ\theta turns, the radius swings out to ∣a∣\lvert a \rvert, back to zero, and out again. Each swing out and back draws one petal.

Example For r=3cos⁡2θr = 3\cos 2\theta the radius is zero at π4\frac{\pi}{4}, 3π4\frac{3\pi}{4}, 5π4\frac{5\pi}{4} and 7π4\frac{7\pi}{4}, a spacing of π2\frac{\pi}{2}.

θ\thetarrPoint (x,y)(x, y)
0033(3,0)(3, 0)
π4\frac{\pi}{4}00(0,0)(0, 0)
π2\frac{\pi}{2}−3-3(0,−3)(0, -3)
3π4\frac{3\pi}{4}00(0,0)(0, 0)
π\pi33(−3,0)(-3, 0)
5π4\frac{5\pi}{4}00(0,0)(0, 0)
3π2\frac{3\pi}{2}−3-3(0,3)(0, 3)
7π4\frac{7\pi}{4}00(0,0)(0, 0)

The rose has four petals of length 33, with tips on the positive and negative xx- and yy-axes, and between the petals it passes through the pole.

Integer angular frequency

Definition In r=acos⁡(nθ)r = a\cos(n\theta) or r=asin⁡(nθ)r = a\sin(n\theta) with n>0n > 0 the number nn is the angular frequency. The radius has period 2πn\frac{2\pi}{n} as a function of θ\theta, so it completes nn full cycles while the direction θ\theta turns once around the pole. When nn is a positive integer, the radius satisfies f(θ+2π)=f(θ)f(\theta + 2\pi) = f(\theta), so after one full turn the point is back where it started and the curve closes up. When nn is not an integer, one turn is not enough. For a fraction such as n=32n = \frac{3}{2} the curve needs more than one turn to close, and for an irrational nn it never closes up. The petal rules below are for integer nn only.

In plain words The angular frequency compares how fast the radius oscillates with how fast the direction turns. With n=3n = 3 the radius goes through three full cosine cycles in one trip around the pole.

Example For r=cos⁡3θr = \cos 3\theta the radius has period 2π3\frac{2\pi}{3} and equals 11 at θ=0\theta = 0, 2π3\frac{2\pi}{3} and 4π3\frac{4\pi}{3}, three petal tips 120∘120^\circ apart. For comparison, r=cos⁡3θ2r = \cos\frac{3\theta}{2} has frequency 32\frac{3}{2}, and after one full turn

cos⁡3(θ+2π)2=cos⁡(3θ2+3π)=−cos⁡3θ2.\begin{aligned} \cos\frac{3(\theta + 2\pi)}{2} &= \cos\left(\frac{3\theta}{2} + 3\pi\right) \\[0.8em] &= -\cos\frac{3\theta}{2}. \end{aligned}

The radius has changed sign, so the curve has not closed. It starts at (1,0)(1, 0) when θ=0\theta = 0 and is at (−1,0)(-1, 0) when θ=2π\theta = 2\pi. It returns to its start only after θ\theta has run through 4π4\pi.

Odd and even petal counts

Definition Let a≠0a \ne 0 and let n≥2n \ge 2 be an integer. The rose r=acos⁡(nθ)r = a\cos(n\theta), and likewise r=asin⁡(nθ)r = a\sin(n\theta), has nn petals when nn is odd and 2n2n petals when nn is even. The reason is the identity

f(θ+π)=(−1)nf(θ),f(\theta + \pi) = (-1)^n f(\theta),

which holds because adding π\pi to θ\theta adds nπn\pi to nθn\theta. For odd nn the name (f(θ+π),θ+π)=(−f(θ),θ+π)(f(\theta + \pi), \theta + \pi) = (-f(\theta), \theta + \pi) is the same point as (f(θ),θ)(f(\theta), \theta), so the second half turn redraws the nn petals of the first. For even nn the second half turn draws the reflections of the first nn petals through the pole, which fall into the gaps between them. The rule applies only to an equation in exactly this form, so rewrite a disguised equation first.

In plain words For odd nn the petals drawn with negative radii land exactly on top of the ones drawn with positive radii, so each petal is drawn twice and you count nn. For even nn they land in the gaps, and you count 2n2n.

Example The rose r=2sin⁡5θr = 2\sin 5\theta has 55 petals, and r=2sin⁡4θr = 2\sin 4\theta has 88. Now take r=4cos⁡2θ−2r = 4\cos^2\theta - 2, which is not in rose form. The power-reducing formula cos⁡2θ=12(1+cos⁡2θ)\cos^2\theta = \frac{1}{2}(1 + \cos 2\theta) gives

r=2(1+cos⁡2θ)−2=2cos⁡2θ,r = 2(1 + \cos 2\theta) - 2 = 2\cos 2\theta,

a rose with 44 petals of length 22. In contrast, r=4cos⁡2θ=2+2cos⁡2θr = 4\cos^2\theta = 2 + 2\cos 2\theta keeps a constant term, so it is not a rose and the rule does not apply. Its radius is never negative, and in [0,2π)[0, 2\pi) it is zero only at θ=π2\theta = \frac{\pi}{2} and 3π2\frac{3\pi}{2}, so the curve has two loops, not four.

Negative radius

Definition When f(θ)<0f(\theta) < 0, the point (f(θ),θ)(f(\theta), \theta) lies at distance ∣f(θ)∣\lvert f(\theta) \rvert from the pole on the ray opposite the direction θ\theta, which is the ray of angle θ+π\theta + \pi. So on a rose, an interval between consecutive zeros where the radius is negative draws a petal on the opposite side of the pole from the directions in that interval.

In plain words A negative radius means walk backward. The angles where rr is negative draw their petal through the pole and out the other side.

Example For r=sin⁡2θr = \sin 2\theta the radius is negative for π2<θ<π\frac{\pi}{2} < \theta < \pi, where θ\theta points into the second quadrant. At θ=3π4\theta = \frac{3\pi}{4} the radius is −1-1, and the point is

(−cos⁡3π4,−sin⁡3π4)=(22,−22),\begin{aligned} &\left(-\cos\frac{3\pi}{4}, -\sin\frac{3\pi}{4}\right) \\[0.8em] &\quad = \left(\frac{\sqrt{2}}{2}, -\frac{\sqrt{2}}{2}\right), \end{aligned}

in the fourth quadrant. So this petal lies in the fourth quadrant, opposite the directions that draw it. The rose has one petal in each quadrant, and two of the four are drawn with negative radii.

Lemniscates

Definition Let a>0a > 0. The graphs of

r2=a2cos⁡2θandr2=a2sin⁡2θ\begin{aligned} r^2 &= a^2\cos 2\theta \quad \text{and} \\[0.4em] r^2 &= a^2\sin 2\theta \end{aligned}

are lemniscates. Each is a figure eight made of two loops that meet at the pole, and each loop reaches distance aa from the pole. The first has its tips at (a,0)(a, 0) and (−a,0)(-a, 0). The second is the first turned through π4\frac{\pi}{4}, since sin⁡2θ=cos⁡2(θ−π4)\sin 2\theta = \cos 2(\theta - \frac{\pi}{4}), and its tips lie on the line y=xy = x. Multiplying the first equation by r2r^2 and using x=rcos⁡θx = r\cos\theta and y=rsin⁡θy = r\sin\theta gives its rectangular form

(x2+y2)2=a2(x2−y2).(x^2 + y^2)^2 = a^2(x^2 - y^2).

Multiplying by r2r^2 could only add the pole, and the pole is already on the curve, at θ=π4\theta = \frac{\pi}{4}.

In plain words Squaring the radius changes the picture. Points exist only where the right side is not negative, and every angle that works gives two opposite points at once.

Example For r2=9cos⁡2θr^2 = 9\cos 2\theta the loops reach (3,0)(3, 0) and (−3,0)(-3, 0). At θ=π6\theta = \frac{\pi}{6} the equation gives r2=92r^2 = \frac{9}{2}, so r=322r = \frac{3\sqrt{2}}{2} is one choice, and the point is

(322cos⁡π6,322sin⁡π6)=(364,324).\begin{aligned} &\left(\frac{3\sqrt{2}}{2}\cos\frac{\pi}{6}, \frac{3\sqrt{2}}{2}\sin\frac{\pi}{6}\right) \\[0.8em] &\quad = \left(\frac{3\sqrt{6}}{4}, \frac{3\sqrt{2}}{4}\right). \end{aligned}

It satisfies the rectangular form, since x2+y2=5416+1816=92x^2 + y^2 = \frac{54}{16} + \frac{18}{16} = \frac{9}{2}, so the left side is 814\frac{81}{4}, and the right side is 9(5416−1816)=8149\left(\frac{54}{16} - \frac{18}{16}\right) = \frac{81}{4} too.

Valid real branches

Definition For an equation r2=g(θ)r^2 = g(\theta), a real radius exists only at the angles where g(θ)≥0g(\theta) \ge 0. At those angles the real values of rr are

r=g(θ)andr=−g(θ),r = \sqrt{g(\theta)} \quad \text{and} \quad r = -\sqrt{g(\theta)},

which are the two real branches. They are different when g(θ)>0g(\theta) > 0 and both equal 00 when g(θ)=0g(\theta) = 0. The graph is everything both branches draw over the angles with g(θ)≥0g(\theta) \ge 0, and the angles with g(θ)<0g(\theta) < 0 give no points. For r2=a2cos⁡2θr^2 = a^2\cos 2\theta the allowed angles in [0,2π)[0, 2\pi) are

0≤θ≤π4,3π4≤θ≤5π4,7π4≤θ<2π.\begin{gathered} 0 \le \theta \le \frac{\pi}{4}, \\[0.8em] \frac{3\pi}{4} \le \theta \le \frac{5\pi}{4}, \\[0.8em] \frac{7\pi}{4} \le \theta < 2\pi. \end{gathered}

In plain words Before you graph, find the angles where the right side is negative and cross them out. On the angles that are left, use both signs of the square root.

Example For r2=4sin⁡2θr^2 = 4\sin 2\theta you need sin⁡2θ≥0\sin 2\theta \ge 0, so 0≤θ≤π20 \le \theta \le \frac{\pi}{2} or π≤θ≤3π2\pi \le \theta \le \frac{3\pi}{2} within [0,2π)[0, 2\pi). On 0≤θ≤π20 \le \theta \le \frac{\pi}{2} the branch r=2sin⁡2θr = 2\sqrt{\sin 2\theta} draws the loop in the first quadrant, with its tip (2,2)(\sqrt{2}, \sqrt{2}) at θ=π4\theta = \frac{\pi}{4}. The branch r=−2sin⁡2θr = -2\sqrt{\sin 2\theta} on the same angles draws the loop in the third quadrant, with its tip (−2,−2)(-\sqrt{2}, -\sqrt{2}). For π2<θ<π\frac{\pi}{2} < \theta < \pi the right side is negative, and these angles give no points.

Tracing interval

Definition A tracing interval for a polar equation is an interval of angles that draws the whole graph, with every real branch included when the equation fixes only r2r^2, and draws no part of it twice, apart from finitely many points such as the pole. For the rose r=acos⁡(nθ)r = a\cos(n\theta) or r=asin⁡(nθ)r = a\sin(n\theta) with an integer n≥2n \ge 2, the interval [0,π)[0, \pi) is a tracing interval when nn is odd, and the full interval [0,2π)[0, 2\pi) is needed when nn is even. For the lemniscate r2=a2cos⁡2θr^2 = a^2\cos 2\theta, the interval [−π4,π4][-\frac{\pi}{4}, \frac{\pi}{4}] with both branches is a tracing interval.

In plain words The tracing interval tells you how far θ\theta must go. Stop too early and you miss petals. Go too far and you draw petals twice, which will matter when you compute areas in calculus.

Example For r=2cos⁡5θr = 2\cos 5\theta the frequency is odd, and

2cos⁡(5(θ+π))=2cos⁡(5θ+5π)=−2cos⁡5θ.\begin{aligned} 2\cos(5(\theta + \pi)) &= 2\cos(5\theta + 5\pi) \\[0.4em] &= -2\cos 5\theta. \end{aligned}

So each angle in [π,2π)[\pi, 2\pi) names a point already drawn by the angle π\pi smaller, and [0,π)[0, \pi) draws all 55 petals once. For r=2cos⁡4θr = 2\cos 4\theta the same shift gives +2cos⁡4θ+2\cos 4\theta, the angles in [π,2π)[\pi, 2\pi) draw the 44 reflected petals, and the full [0,2π)[0, 2\pi) is needed for all 88.

Check yourself

  1. How many petals does r=5sin⁡6θr = 5\sin 6\theta have, how long are they, and what interval of θ\theta traces the rose once?
Show the answer

The frequency 66 is even, so there are 1212 petals, each of length 55. The interval [0,2π)[0, 2\pi) is needed to draw them all once.

  1. Find the petal tips of r=4cos⁡3θr = 4\cos 3\theta as rectangular points, and give an interval that traces the rose once.
Show the answer

The radius is 44 at θ=0\theta = 0, 2π3\frac{2\pi}{3} and 4π3\frac{4\pi}{3}, which gives the tips

(4,0),(−2,23),(−2,−23).\begin{gathered} (4, 0), \\[0.4em] (-2, 2\sqrt{3}), \\[0.4em] (-2, -2\sqrt{3}). \end{gathered}

The radius −4-4 at θ=π3\theta = \frac{\pi}{3} names the same point as (4,4π3)(4, \frac{4\pi}{3}), so it adds no new tip. The frequency is odd, so [0,π)[0, \pi) traces the rose once.

  1. For r2=16cos⁡2θr^2 = 16\cos 2\theta, which angles in [0,2π)[0, 2\pi) give points, and where does the graph meet the xx-axis?
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Points exist where cos⁡2θ≥0\cos 2\theta \ge 0, that is for

0≤θ≤π4,3π4≤θ≤5π4,7π4≤θ<2π.\begin{gathered} 0 \le \theta \le \frac{\pi}{4}, \\[0.8em] \frac{3\pi}{4} \le \theta \le \frac{5\pi}{4}, \\[0.8em] \frac{7\pi}{4} \le \theta < 2\pi. \end{gathered}

At θ=0\theta = 0 the radius is ±4\pm 4, which gives (4,0)(4, 0) and (−4,0)(-4, 0). The graph also passes through the pole, at θ=π4\theta = \frac{\pi}{4}. So it meets the xx-axis at (−4,0)(-4, 0), the origin and (4,0)(4, 0).

How this lesson connects